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Spectroscopic and photoluminescence studies of a wide band gap insulating material : Powdered and colloidal ZrO2 sols. / Emeline, Alexei; Kataeva, Galina V.; Litke, Alexander S.; Rudakova, Aida V.; Ryabchuk, Vladimir K.; Serpone, Nick.

In: Langmuir, Vol. 14, No. 18, 01.09.1998, p. 5011-5022.

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@article{74b7a5bf5d6c473e86522077fbae874e,
title = "Spectroscopic and photoluminescence studies of a wide band gap insulating material: Powdered and colloidal ZrO2 sols",
abstract = "Powdered zirconia and colloidal zirconia aqueous sols have been examined by diffuse reflectance and absorption spectroscopies and by photoluminnescence methods in solid/gas systems. The former system was examined following high-temperature treatment in vacuo and under reducing and oxidizing atmospheres. Studies of the influence of H2 and O2 on the photophysics of microparticles (powder) and nanoparticles (colloidal sols) of zirconia at solid/gas interfaces and the effect of free carrier scavengers (CH3OH and O2) on the photophysic at solid/liquid interfaces were undertaken to explore the correlation between surface chemistry and the nature of preexisting or photogenerated defect centers (e.g., F-type and V-type color centers). ZrO2 is an insulating, direct wide gap metal oxide with an optical band gap of ∼5.0 eV; another optical transition occurs at 5.85 eV. The optical behavior depends on whether zirconia is preirradiated in the intrinsic (hv > 5.0 eV) or extrinsic (hv < 5.0 eV) absorption regions. The red limits of the effect are 3.0 and 3.2eV for microparticles and nanoparticles respecttively. New defects are formed by the photoionization of, and/or by free carrier trapping by, existing defects. New defects formed by tunneling electron transfer from donor to acceptor defect states in zironia nanoparticles are not precluded. Regardless of the type of mechanism, the influence of surface chemical reactions on the formation of defect centers is typical of both systems which luminesce under irradiation. Powdered ZrO2 shows a decrease in luminescence the longer it is irradiated Emission decay in ZrO2 sols depends on whether the sols were preirradiated in the intrinsic or extrinsic regions; luminescence intensity was affected by the type of carrier scavengers present (methanol or oxygen). Different origins have been identified for the decay of emission: (i) for powdered ZrO2 samples, nonradiative recombination of free electrons with photogenerated hole centers after preirradiation with UV light; (ii) for preirradiated colloidal ZrO2 sels, photoionization of, and recombination of free carriers with, emissive defect centers.",
author = "Alexei Emeline and Kataeva, {Galina V.} and Litke, {Alexander S.} and Rudakova, {Aida V.} and Ryabchuk, {Vladimir K.} and Nick Serpone",
year = "1998",
month = sep,
day = "1",
language = "English",
volume = "14",
pages = "5011--5022",
journal = "Langmuir",
issn = "0743-7463",
publisher = "American Chemical Society",
number = "18",

}

RIS

TY - JOUR

T1 - Spectroscopic and photoluminescence studies of a wide band gap insulating material

T2 - Powdered and colloidal ZrO2 sols

AU - Emeline, Alexei

AU - Kataeva, Galina V.

AU - Litke, Alexander S.

AU - Rudakova, Aida V.

AU - Ryabchuk, Vladimir K.

AU - Serpone, Nick

PY - 1998/9/1

Y1 - 1998/9/1

N2 - Powdered zirconia and colloidal zirconia aqueous sols have been examined by diffuse reflectance and absorption spectroscopies and by photoluminnescence methods in solid/gas systems. The former system was examined following high-temperature treatment in vacuo and under reducing and oxidizing atmospheres. Studies of the influence of H2 and O2 on the photophysics of microparticles (powder) and nanoparticles (colloidal sols) of zirconia at solid/gas interfaces and the effect of free carrier scavengers (CH3OH and O2) on the photophysic at solid/liquid interfaces were undertaken to explore the correlation between surface chemistry and the nature of preexisting or photogenerated defect centers (e.g., F-type and V-type color centers). ZrO2 is an insulating, direct wide gap metal oxide with an optical band gap of ∼5.0 eV; another optical transition occurs at 5.85 eV. The optical behavior depends on whether zirconia is preirradiated in the intrinsic (hv > 5.0 eV) or extrinsic (hv < 5.0 eV) absorption regions. The red limits of the effect are 3.0 and 3.2eV for microparticles and nanoparticles respecttively. New defects are formed by the photoionization of, and/or by free carrier trapping by, existing defects. New defects formed by tunneling electron transfer from donor to acceptor defect states in zironia nanoparticles are not precluded. Regardless of the type of mechanism, the influence of surface chemical reactions on the formation of defect centers is typical of both systems which luminesce under irradiation. Powdered ZrO2 shows a decrease in luminescence the longer it is irradiated Emission decay in ZrO2 sols depends on whether the sols were preirradiated in the intrinsic or extrinsic regions; luminescence intensity was affected by the type of carrier scavengers present (methanol or oxygen). Different origins have been identified for the decay of emission: (i) for powdered ZrO2 samples, nonradiative recombination of free electrons with photogenerated hole centers after preirradiation with UV light; (ii) for preirradiated colloidal ZrO2 sels, photoionization of, and recombination of free carriers with, emissive defect centers.

AB - Powdered zirconia and colloidal zirconia aqueous sols have been examined by diffuse reflectance and absorption spectroscopies and by photoluminnescence methods in solid/gas systems. The former system was examined following high-temperature treatment in vacuo and under reducing and oxidizing atmospheres. Studies of the influence of H2 and O2 on the photophysics of microparticles (powder) and nanoparticles (colloidal sols) of zirconia at solid/gas interfaces and the effect of free carrier scavengers (CH3OH and O2) on the photophysic at solid/liquid interfaces were undertaken to explore the correlation between surface chemistry and the nature of preexisting or photogenerated defect centers (e.g., F-type and V-type color centers). ZrO2 is an insulating, direct wide gap metal oxide with an optical band gap of ∼5.0 eV; another optical transition occurs at 5.85 eV. The optical behavior depends on whether zirconia is preirradiated in the intrinsic (hv > 5.0 eV) or extrinsic (hv < 5.0 eV) absorption regions. The red limits of the effect are 3.0 and 3.2eV for microparticles and nanoparticles respecttively. New defects are formed by the photoionization of, and/or by free carrier trapping by, existing defects. New defects formed by tunneling electron transfer from donor to acceptor defect states in zironia nanoparticles are not precluded. Regardless of the type of mechanism, the influence of surface chemical reactions on the formation of defect centers is typical of both systems which luminesce under irradiation. Powdered ZrO2 shows a decrease in luminescence the longer it is irradiated Emission decay in ZrO2 sols depends on whether the sols were preirradiated in the intrinsic or extrinsic regions; luminescence intensity was affected by the type of carrier scavengers present (methanol or oxygen). Different origins have been identified for the decay of emission: (i) for powdered ZrO2 samples, nonradiative recombination of free electrons with photogenerated hole centers after preirradiation with UV light; (ii) for preirradiated colloidal ZrO2 sels, photoionization of, and recombination of free carriers with, emissive defect centers.

UR - http://www.scopus.com/inward/record.url?scp=0032162724&partnerID=8YFLogxK

M3 - Article

AN - SCOPUS:0032162724

VL - 14

SP - 5011

EP - 5022

JO - Langmuir

JF - Langmuir

SN - 0743-7463

IS - 18

ER -

ID: 35145527